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(1)(2)Objectives • deals with forces applied by fluids at rest or in rigid-body motion

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The fluid property responsible for those forces is pressure, which is a normal force exerted by a fluid per unit area. Analyze the variation of pressure in liquids undergoing linear acceleration and in rotating containers. The actual pressure at a given position is called absolute pressure and is measured relative to absolute vacuum (i.e. absolute zero pressure).

Pressure definition

Pressure at point

In the absence of shear forces, this result can be shown to be applicable to fluids in motion as well as fluids at rest.

Pressure variation

The pressure in a fluid increases with depth because more fluid resides in deeper layers, and the effect of this "extra weight" in a deeper layer is balanced by an increase in pressure.

Pressure Measurement

Pascal's law: 2 points at the same height in a continuous fluid at rest are at the same pressure. Manometers are particularly suitable for measuring pressure drop across a horizontal flow section between two specified points due to the presence of a device such as a valve or heat exchanger or any resistance to flow. The Italian EvangelistaTorricelli was the first to prove conclusively that the atmospheric pressure can be measured by inverting a.

If water instead of mercury were used to measure standard atmospheric pressure, a water column of about 10.3 m would be required. Epistaxis is a common experience at high altitudes, as the difference between blood pressure and atmospheric pressure is greater at this.

Hydrostatic Forces On Submerged Surfaces

The pressure P0 is usually atmospheric pressure, which in most cases can be ignored as it acts on both sides of the plate. Then assume the presence of an additional liquid layer of the thickness on top of the liquid with absolute vacuum above. The line of action of the resulting hydrostatic force generally does not pass through the center of gravity of the surface.

Ixx are commonly available for common shapes in engineering handbooks, but they are usually given about the axes passing through the centroid of the area. The exact location of the line of action of the resultant force (eg, its distance from one of the endpoints of the curved surface) can be determined by taking an instant about a suitable point. The hydrostatic force acting on a circular surface always passes through the center of the circle, as the pressure forces are.

The line of action of this equivalent force can be determined from the requirement that the moment of the equivalent force about any point is equal to the sum of the moments of the individual forces about the same point.

Buoyancy

The weight and the buoyant force must have the same line of action to have a zero torque: Archimedes' principle. The buoyant force acting on a body immersed in a fluid is equal to the weight of the fluid displaced by the body, and it acts upward through. center of gravity of the displaced volume. the weight of the whole body must be equal to. The buoyant force is proportional to the density of the liquid and therefore we can believe that the buoyant force exerted by gases such as air is negligible.

For example, the volume of a person is about 0.1 m3, and if we take the density of air to be 1.2 kg/m3, so is the buoyancy force that air exerts on the person.

Buoyancy & Stability

Stability

For a submerged or floating body in static equilibrium, the weight and the buoyant force acting on the body balance each other, and such bodies are inherently stable in the vertical direction. If a submerged, neutrally buoyant body is raised or lowered to a different depth, the body will remain in equilibrium at that location. If a floating body is raised or lowered somewhat by a vertical force, the body will return to its original position as soon as the external effect is removed.

Therefore, a floating body possesses vertical stability, while a neutrally submerged floating body is neutrally stable, as it does not return to its original position after a disturbance.

Stability: Immersed body

Stable: A rotational disturbance of the body in such cases produces a recovery moment to return the body to its original stable position. A submerged body whose center of gravity G is directly above point B is unstable and any disturbance will cause this body to turn upside down. What about a case where the center of gravity is not vertically aligned with the center of gravity.

Stability: Floating body

If point B' is far enough, these two forces create a restoring moment and return the body to its original position. A floating body is stable if point M is above point G and therefore GM is positive, and unstable if point M is below point G and therefore GM is negative. The measure of stability of floating bodies is the metacentric height GM. The measure of stability of floating bodies is the metacentric height GM.

The metacenter can be considered a fixed point for small roll angles of up to about 20°. In the latter case, the weight and buoyancy acting on the tilted body generate a tipping moment instead of a recovery moment, causing the body to capsize. Length of the metacentric height GM above G is a measure of stability: the larger it is, the more stable the buoyancy body is.

Fluids in Rigid-body Motion

Fluids in Rigid-body Motion: Straight path

Fluids in Rigid-body Motion: Cylindrical container

We thus conclude that the surfaces of constant pressure, including the free surface, are paraboloids of revolution. Where hc is the distance of the free surface from the bottom of the container along the axis of rotation. Zs is the distance from the free surface to the bottom of the container at radius r.

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